%0 Journal Article %T Intermittency Route to Strange Nonchaotic Attractors %A Awadhesh Prasad %A Vishal Mehra %A Ramakrishna Ramaswamy %J Physics %D 1997 %I arXiv %R 10.1103/PhysRevLett.79.4127 %X Strange nonchaotic attractors (SNA) arise in quasiperiodically driven systems in the neighborhood of a saddle node bifurcation whereby a strange attractor is replaced by a periodic (torus) attractor. This transition is accompanied by Type-I intermittency. The largest nontrivial Lyapunov exponent $\Lambda$ is a good order-parameter for this route from chaos to SNA to periodic motion: the signature is distinctive and unlike that for other routes to SNA. In particular, $\Lambda$ changes sharply at the SNA to torus transition, as does the distribution of finite-time or N--step Lyapunov exponents, P(\Lambda_N). %U http://arxiv.org/abs/chao-dyn/9709035v1